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Material<br />
Y 2O 3 / lr<br />
W<br />
Re<br />
Relative intensity<br />
www.pfeiffer-vacuum.net<br />
100 %<br />
5<br />
CO 2 <strong>Vacuum</strong><br />
10<br />
5<br />
1<br />
5<br />
0.1<br />
5<br />
0.01<br />
10 12 14 16 18 20 22 24 26 28 30 32 34 36 38 40 42 44 46 48 amu<br />
Figure 4.7: Fractal ion distribution of CO 2<br />
Table 4.1: Filament materials and their employment<br />
Temperature<br />
1,300 °C<br />
1,800 °C<br />
1,800 °C<br />
Applicable Gases<br />
Inert gases, Air / O2, NOx, SOx Inert gases, H2, halogens, freons<br />
Inert gases,<br />
hydrocarbons, H2, halogens, freons<br />
Remarks<br />
Mass number<br />
Short service life with halogens, insensitive to<br />
high O2 concentrations,<br />
generates some CO / CO2 from O2 or H2O background<br />
Short service life with O2 applications,<br />
generates some CO / CO2 from O2 or H2O background,<br />
C causes brittleness<br />
Service life around three months due to<br />
vaporization of the material,<br />
used in connection with hydrocarbons<br />
The various ion sources are described below on the basis of their attributes and fields of<br />
application. What all ions have in common is that they can be electrically biased up to 150 V.<br />
This avoids signal background due to ESD ions. This technology will be explained in<br />
detail later.<br />
Axial ion source<br />
This ion source is characterized by its extremely robust mechanical design and high sensitivity.<br />
It is primarily employed for residual gas analysis in high vacuum systems due to its open<br />
construction. Figure 4.8 shows a schematic diagram of an axial ion source.<br />
Page 95<br />
<strong>Technology</strong>